EP1966615A1 - Device, probe, and method for the galvanically decoupled transmission of a measuring signal - Google Patents
Device, probe, and method for the galvanically decoupled transmission of a measuring signalInfo
- Publication number
- EP1966615A1 EP1966615A1 EP06830608A EP06830608A EP1966615A1 EP 1966615 A1 EP1966615 A1 EP 1966615A1 EP 06830608 A EP06830608 A EP 06830608A EP 06830608 A EP06830608 A EP 06830608A EP 1966615 A1 EP1966615 A1 EP 1966615A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- signal
- transceiver
- sensor
- microwave signal
- probe
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 239000000523 sample Substances 0.000 title claims abstract description 46
- 230000005540 biological transmission Effects 0.000 title claims abstract description 34
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- 230000010287 polarization Effects 0.000 claims description 8
- 238000011156 evaluation Methods 0.000 claims description 7
- 230000001419 dependent effect Effects 0.000 claims description 6
- 230000008859 change Effects 0.000 claims description 4
- 239000004065 semiconductor Substances 0.000 claims description 4
- 239000000758 substrate Substances 0.000 claims description 4
- 230000003287 optical effect Effects 0.000 description 7
- 239000004020 conductor Substances 0.000 description 5
- 230000001965 increasing effect Effects 0.000 description 4
- 230000005855 radiation Effects 0.000 description 4
- 238000012360 testing method Methods 0.000 description 4
- 238000001514 detection method Methods 0.000 description 3
- 239000000835 fiber Substances 0.000 description 3
- 238000002955 isolation Methods 0.000 description 3
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- 241001422033 Thestylus Species 0.000 description 2
- 238000009529 body temperature measurement Methods 0.000 description 2
- 238000013461 design Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 230000001939 inductive effect Effects 0.000 description 2
- 230000005693 optoelectronics Effects 0.000 description 2
- 230000001681 protective effect Effects 0.000 description 2
- 230000008054 signal transmission Effects 0.000 description 2
- 229910018072 Al 2 O 3 Inorganic materials 0.000 description 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 230000009471 action Effects 0.000 description 1
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- 238000010079 rubber tapping Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 230000009131 signaling function Effects 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R15/00—Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
- G01R15/14—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
- G01R15/26—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using modulation of waves other than light, e.g. radio or acoustic waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R1/00—Details of instruments or arrangements of the types included in groups G01R5/00 - G01R13/00 and G01R31/00
- G01R1/02—General constructional details
- G01R1/06—Measuring leads; Measuring probes
- G01R1/067—Measuring probes
- G01R1/06777—High voltage probes
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R1/00—Details of instruments or arrangements of the types included in groups G01R5/00 - G01R13/00 and G01R31/00
- G01R1/02—General constructional details
- G01R1/06—Measuring leads; Measuring probes
- G01R1/067—Measuring probes
- G01R1/06788—Hand-held or hand-manipulated probes, e.g. for oscilloscopes or for portable test instruments
Definitions
- the invention relates to a device, a probe and a method for galvanically decoupled transmission of a measuring signal with the features mentioned in the preamble of claims 1, 19 and 22.
- assemblies and devices signals In the development and testing of electrical or electronic components, assemblies and devices signals must be taken from any point of a test specimen.
- oscilloscopes are often used for acquisition and graphical representation. Since almost all oscilloscopes are desktop devices, they can not be contacted directly with the DUT, using probes.
- a probe is a measuring adapter for connecting a measuring device to a measuring point in a circuit.
- the task of the probe is the most unadulterated transmission of the measured value, if possible without noticeable influence on the test object.
- An oscilloscope probe consists of the following parts: A probe tip for contacting the measuring signal on a conductor, contacts of a component or the like. ; a short, flexible wire with clamp for tapping the reference potential of the
- Measurement signal a probe body for holding by hand; and cables and connectors for transmitting the measurement signal to the oscilloscope.
- Oscilloscope ie low distortion of the waveform and low amplitude errors and a high dynamic range can be mentioned here.
- the reference potential of the measuring signal is looped through by the measuring object to the oscilloscope (oscilloscope reference potential).
- this pole of the oscilloscope is connected to the housing and further to the protective conductor of the power supply network.
- the reference potentials of the measuring signals are connected to each other via the oscilloscope.
- test object has several reference potentials for the measuring signals and these must not be connected with each other or with the protective conductor of the power supply network, then such measurements were not necessary.
- Galvanic isolation means the case that there is no way for carriers to flow from one circuit to another, immediately adjacent circuit.
- the most common application for galvanic isolation are transformers connected to the public grid.
- a galvanic separation is prescribed, which are realized by two electrically separate coils with a common iron core.
- differential probes and optoelectronic probe systems realize a "virtual" or true decoupling of measurement signal and oscilloscope. Where decoupling of the measurement signal from the oscilloscope is not required, probes will be used where the measurement signal reference potential is looped through to the oscilloscope. The latter are above all more cost-effective than commercially available differential probes or optoelectronic probe systems.
- Differential probes work according to the following principle: The output signal of two styli is placed on a differential amplifier located in the probe. Or two probes are connected via lines to a differential amplifier. The differential amplifier output is connected to the oscilloscope. Ideally, the difference signals isolate the two differential signals completely from the reference potential of the oscilloscope.
- a disadvantage of these systems is a finite common-mode input voltage range. The finite common mode input voltage range of the differential amplifier limits the amplitude of the common mode signal. Furthermore, the common-mode negative pressure decreases with increasing frequency of the common-mode signal. While with common-frequency signals of low frequency (eg 50 Hz) even with low-cost differential
- the radiation is disadvantageous in differential probes.
- the two probes are connected via cables to the Differenzverstarker.
- parts of the measurement signal and its reference potential (common-mode signal) are radiated into the environment.
- the radiation With increasing frequency and amplitude of the common-mode signal, the radiation increases. This radiation loads the measuring signal and its reference potential, it is unintentionally changed, and the measured value no longer represents the signal to be measured in the undisturbed state even with perfect transmission of the signal.
- Oscilloscope is connected, improve.
- the disadvantage, however, is that these solutions are very expensive.
- systems with optical transmission of the measurement signal are known.
- the measurement signal is modulated onto an optical carrier, for example by modulation of the radiation power of a semiconductor laser diode.
- the modulated light is transmitted via a glass fiber.
- the receiver for example, it is demodulated again by means of a photodiode. This method allows a virtually complete decoupling of the measurement signal from the oscilloscope.
- the optical signal is neither susceptible nor disturbing.
- DE 101 01 632 B4 discloses an oscilloscope probe with a fiber optic sensor for potential-free detection of electrical variables.
- WO 89/09413 A1 describes an oscilloscope probe with a fiber optic sensor for potential-free detection of electrical variables.
- the sensor head has an electro-optical crystal, by means of which light supplied to it is influenced by a polarization by the action of an electric field. The difference between the original polarization and the changed polarization is then converted into an electrical quantity. Fiber optic cables are used during transmission.
- a measuring head for the potential-free and storefree detection of the intensity of an electric field or of the absolute value of a voltage is disclosed in US Pat. No. 5,465,043. Again, the change in light polarization reflects the field strength or the voltage value.
- WO 89/09413 A1 requires in the probe an optical system which has elements to be mechanically fastened and to be adjusted with respect to its axis, such as a beam splitter, a mirror and lenses, and in DE 101 01 632 B4 an expensive electro-optical sensor is used.
- Inductive transmission modes are limited in the dielectric strength and produce a parasitic capacitive coupling between the sensor and the evaluation device.
- the problem is inventively solved by the fact that a microwave signal is given by a transceiver via a galvanically decoupling waveguide to a sensor.
- this signal is partially reflected, wherein the amplitude and / or phase of the reflected microwave signal contains the information about the measured value.
- the reflected microwave signal passes through the same waveguide back to the transceiver and is evaluated in this.
- This is a simple and cost-effective design, which requires no power supply, in particular on the sensor side in general by the use of reflection.
- the sensor can also be realized in a very compact manner, which minimizes the influence of the sensor on the measuring signal. When used as a potential separate probe for oscilloscopes, this design allows for easy handling.
- a device for the galvanically decoupled transmission of a measuring signal to a transceiver for microwaves, which is connected via a means for galvanically decoupled transmission of microwaves with a sensor.
- the means for the galvanically decoupled transmission of microwaves is a dielectric waveguide or a waveguide with a plurality of electroconductive conductor pieces, which are connected in isolation from one another.
- the transceiver is a continuous wave (CW) Signal Transceiver, a transceiver for amplitude modulated, including pulsed microwave signals, a transceiver for frequency modulated microwave signals or a transceiver for microwave signals, consisting of several superimposed frequencies.
- the transceiver includes an oscillator and a demodulator.
- the demodulator is preferably designed as a mixer between the oscillator signal and the reflected signal.
- the sensor may be an electrical signal sensor or a non-electrical signal sensor. If the sensor receives a non-electrical measurement signal, it converts it into an electrical measurement signal.
- the sensor includes a reflector and an element that modifies the reflection in a manner characterizing the measurement signal (modulator).
- the modulator has a semiconductor diode, a transistor or a temperature-dependent resistor.
- the means for transmitting the microwave signal is integrated together with the transceiver and the sensor on a substrate. This allows the miniaturization of the device.
- the inventive probe for the galvanically decoupled transmission of measurement signals consisting of a
- Tastspitze a Tastkopfkorper with a housing and a connection to a measuring device is characterized in that the probe according to the invention above Device for the galvanically decoupled transmission of a measuring signal, comprising a transceiver for microwaves, which is connected via a means for the galvanically decoupled transmission of microwaves with a sensor.
- the stylus tip has a stylus and an input circuit.
- the probe further includes an amplifier disposed between the transceiver and the connection to a meter. Furthermore, the probe may have a microcontroller which is connected to the amplifier.
- a method for the galvanically decoupled transmission of a measurement signal comprises the steps of: transmitting a microwave signal from a transceiver, transmitting the microwave signal from the transceiver via a galvanic decoupling means for transmitting microwaves to a sensor, reflecting the signal in Sensor, wherein the microwave signal is changed in a manner characterizing the measured value, transmitting the reflected microwave signal from the sensor via the galvanic decoupling means for transmitting microwaves to the transceiver, and evaluation of the reflected microwave signal in the transceiver.
- the reflected microwave signal is in the transceiver in terms of amplitude, phase, polarization or a combination of amplitude, phase and
- the signal is significantly less loaded during the measurement and can thus be measured unadulterated.
- Fig. 1 The inventive device for the galvanically decoupled transmission of signals in a schematic overview.
- Fig. 2 A schematic detail view of the device according to the invention in an exemplary embodiment for voltage measurement.
- Fig. 3 A schematic detail view of the sensor of the inventive device in an exemplary embodiment for temperature measurement.
- FIG. 4 shows a schematic view of a probe according to the invention.
- the arrangement of FIG. 1 consists of a transceiver 1, a means for galvanically decoupled transmission of microwaves and a sensor 3.
- the means for transmitting microwaves as a dielectric waveguide 2 is realized.
- the transceiver 1 generates a microwave signal and evaluates the signal reflected by the sensor 3. It contains an oscillator for the desired microwave frequency.
- the reflected microwave signal can be multiplied by a mixer with the oscillator signal and provides a DC signal, which depends on the amplitude and phase of the reflection.
- the means for the galvanically decoupled transmission of microwaves can, for example, as a dielectric
- Waveguide 2 can be realized.
- a shield can be provided.
- the sensor 3 contains a reflector 17 and a modulator for changing the characteristics of the reflector 17.
- the measurement signal influences the impedance of the modulator and thus the reflection properties of the reflector 17.
- the preferred embodiment of the sensor 3 for voltage measurement is shown in FIG.
- the waveguide 2 is connected to the reflector 17 and this with the drain-source channel of a transistor 6.
- An electrical input 7 is formed by the gate and source of the transistor 6. At this input 7, an electrical signal is applied, via the
- FIG. 1 A further realization possibility of the sensor 3 for temperature measurement is shown in FIG. One
- Transition element 4 connects the waveguide 2 with the
- Fig. 4 shows a schematic view of the inventive probe.
- the outer shape of the probe corresponds approximately to that of a fountain pen.
- Transceiver 1, microwave conductor 2 and sensor 3 form a mechanical unit.
- the functional units of the probe are a means for contacting the measurement signal, preferably a probe tip 8, the sensor 3, the transceiver 1, the means for transmitting microwaves and the amplifier 9 and possibly a microcontroller 10.
- the probe tip 8 can also be replaced be educated.
- the stylus tip 8 preferably contains a stylus 13 and a short, flexible cable with mini-clamp or two styli, which contact the measuring signal and its reference potential.
- the styli (or stylus 13 + flexible line) are connected to an input circuit 14.
- the input circuit 14 contains elements for attenuating the measurement signal, for correcting the frequency response and for protecting the active element following in the signal path, see sensor 3.
- the reflector 17 is a symmetrical dipole
- the active element is a MOSFET. Its drain and source are each contacted with one leg of the dipole antenna. At the gate and source is measured signal and reference potential. The gate-source voltage changing with the measuring signal modulates the channel resistance of the MOSFETs. The MOSFET channel above the dipole's bottom closes the dipole more or less short. As a result, the phase and amplitude of the reflected wave are changed as a function of the measurement signal.
- the transceiver 1 includes in a preferred embodiment, a microwave oscillator 15 and a mixer and demodulator 16.
- the generated in the oscillator 15 RF energy is passed to a part of the sensor or reflector 17, on the other hand given to the mixer 16.
- the reflected wave is superimposed nonlinearly in the mixer 16 of the oscillator oscillation. If the phase and / or amplitude of the reflected wave changes, the demodulator 16 generates a changing voltage.
- the means for transmitting microwaves is preferably a dielectric waveguide 2. It passes the microwave from the oscillator 15 to the sensor / reflector 3 and back to the mixer 16.
- the dielectric waveguide 2 isolates the measuring signal from the connected oscilloscope (not shown).
- the amplifier 9 amplifies the voltage applied to the demodulator 16.
- it can contain non-linear elements and switching elements.
- the non-linear elements can compensate for nonlinearities in the signal path (caused by MOSFETs, sensor 3 and demodulator 16) and thus the increase usable dynamic range.
- switching elements can be present, which serve for zero and gain adjustment. These can be controlled by a microcontroller 10.
- microcontroller 10 controls the microcontroller 10
- the output impedance of the amplifier 9 is adapted to the line to the oscilloscope 11.
- the use of microwaves over light waves allows the device and probe to be miniaturized.
- the measuring sensor has a size of about 0.1 cm 3 in one embodiment. This allows a cheaper version.
- the device can be manufactured integrated on a substrate. For example, the methods of thin-film technology can be applied to an Al 2 O 3 substrate. Also, the immunity of the device is increased by the miniaturization.
- the device according to the invention allows the bandwidth of the measurement signal to be increased compared to lightwave applications.
- the microwave frequency is preferably between 12 to 30 GHz.
- the load of the measurement object is also very small, typically less than 1 pF.
- broadband measurements at high-impedance measuring points for example, source impedances of 1 kOhm
- electrical signals can also be measured in strongly electromagnetic interference environments. The use of different reference potentials is not a problem.
- the measurement is not by the storage capacity of a battery, as in the
- Signal transmission via optical fiber needed, limited. Both analog and digital signals can be measured. Shortest pulses are measurable.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Measuring Leads Or Probes (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102005061683A DE102005061683B4 (en) | 2005-12-21 | 2005-12-21 | Device, probe and method for the galvanically decoupled transmission of a measurement signal |
PCT/EP2006/069684 WO2007071608A1 (en) | 2005-12-21 | 2006-12-13 | Device, probe, and method for the galvanically decoupled transmission of a measuring signal |
Publications (2)
Publication Number | Publication Date |
---|---|
EP1966615A1 true EP1966615A1 (en) | 2008-09-10 |
EP1966615B1 EP1966615B1 (en) | 2013-11-27 |
Family
ID=37836644
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP06830608.3A Not-in-force EP1966615B1 (en) | 2005-12-21 | 2006-12-13 | DEVICE and PROBE FOR THE GALVANICALLY DECOUPLED TRANSMISSION OF A MEASURING SIGNAL |
Country Status (4)
Country | Link |
---|---|
US (1) | US7893683B2 (en) |
EP (1) | EP1966615B1 (en) |
DE (1) | DE102005061683B4 (en) |
WO (1) | WO2007071608A1 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5082335B2 (en) * | 2006-08-21 | 2012-11-28 | 富士通株式会社 | Electronic board and backboard transmission method |
DE102009019039A1 (en) | 2009-04-27 | 2010-11-11 | Rohde & Schwarz Gmbh & Co. Kg | Measuring device and measuring method for measuring differential signals |
EP3542136B1 (en) * | 2016-11-15 | 2023-10-25 | Ohio State Innovation Foundation | Antenna-coupled radio frequency (rf) probe with a replaceable tip |
US10996178B2 (en) * | 2017-06-23 | 2021-05-04 | Tektronix, Inc. | Analog signal isolator |
CN113608037B (en) * | 2021-08-09 | 2022-06-17 | 西安电子科技大学 | Pulse electric field sensor based on asymmetric straight waveguide interferometer |
Family Cites Families (21)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
ZA704856B (en) | 1969-08-06 | 1971-06-30 | Siemens Ag | Improvements in or relating to arrangements for measuring currents in high tension conductors |
US3805198A (en) * | 1972-08-28 | 1974-04-16 | Bell Telephone Labor Inc | Resonance control in interdigital capacitors useful as dc breaks in diode oscillator circuits |
CA1060098A (en) * | 1976-12-09 | 1979-08-07 | Stanislaw S. Stuchly | System for monitoring and measuring high voltage d.c. transmission line current |
US4392074A (en) * | 1980-09-19 | 1983-07-05 | Siemens Aktiengesellschaft | Trigger device and piezo-ignition coupler with galvanic decoupling |
WO1989009413A1 (en) * | 1988-03-25 | 1989-10-05 | Princeton Applied Research Corporation | Electro-optic probe |
US5273610A (en) * | 1992-06-23 | 1993-12-28 | Association Institutions For Material Sciences, Inc. | Apparatus and method for determining power in plasma processing |
JPH06102295A (en) * | 1992-07-28 | 1994-04-15 | Hewlett Packard Co <Hp> | Non-contact type probe and non-contact voltage measuring device |
EP0668507B1 (en) * | 1993-07-07 | 2002-10-09 | NEC TOKIN Corporation | Electric field sensor |
EP0696739B1 (en) * | 1994-08-12 | 2002-11-20 | Matsushita Electric Industrial Co., Ltd. | Optical sensor |
US5923175A (en) | 1997-06-03 | 1999-07-13 | The United States Of America As Represented By The Secretary Of The Navy | Apparatus for contactless measurement of the electrical resistance of a conductor |
SE515783C2 (en) * | 1997-09-11 | 2001-10-08 | Ericsson Telefon Ab L M | Electrical devices and process for their manufacture |
GB2342161B (en) * | 1998-09-30 | 2000-12-20 | Ando Electric | Electro-optic probe |
DE19955978C2 (en) | 1998-11-24 | 2002-06-27 | Ando Electric | Electro-optical probe for an oscilloscope that measures a signal waveform |
DE19933978A1 (en) * | 1999-07-20 | 2001-01-25 | Abb Research Ltd | Transponder-based wireless information transfer method, e.g. for process variables or actuator commands, involves substation performing phase modulation of received HF signal and reflecting modulated narrow band signal back to base station |
DE10010846A1 (en) | 2000-03-06 | 2001-09-20 | Siemens Ag | Appliance for determining measured variables corresponding to reactive resistance of sensor connected to surface acoustic wave (SAW) element matching network |
DE20011084U1 (en) * | 2000-06-23 | 2000-10-05 | Schumann Mathias | Oscilloscope probe with fiber optic sensor for potential-free detection of electrical quantities |
JP4265206B2 (en) * | 2002-11-27 | 2009-05-20 | 株式会社 東北テクノアーチ | Non-contact conductivity measurement system |
WO2004109583A1 (en) * | 2003-06-06 | 2004-12-16 | Stemco Llc | Wireless communication device, system for communication and communication method |
DE10361991A1 (en) * | 2003-09-27 | 2005-04-28 | Univ Hamburg Harburg Tech | Telemetrically interrogated passive potential sensor |
DE102004014563B4 (en) * | 2004-03-25 | 2011-01-13 | Atmel Automotive Gmbh | Method and device for improved wireless data transmission |
US7859071B2 (en) * | 2005-03-31 | 2010-12-28 | Finisar Corporation | Power and communication interface for sensors using a single tethered fiber |
-
2005
- 2005-12-21 DE DE102005061683A patent/DE102005061683B4/en not_active Expired - Fee Related
-
2006
- 2006-12-13 EP EP06830608.3A patent/EP1966615B1/en not_active Not-in-force
- 2006-12-13 WO PCT/EP2006/069684 patent/WO2007071608A1/en active Application Filing
- 2006-12-13 US US12/158,785 patent/US7893683B2/en not_active Expired - Fee Related
Non-Patent Citations (1)
Title |
---|
See references of WO2007071608A1 * |
Also Published As
Publication number | Publication date |
---|---|
DE102005061683B4 (en) | 2011-12-08 |
EP1966615B1 (en) | 2013-11-27 |
US20080290856A1 (en) | 2008-11-27 |
DE102005061683A1 (en) | 2007-07-19 |
US7893683B2 (en) | 2011-02-22 |
WO2007071608A1 (en) | 2007-06-28 |
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